2016
DOI: 10.1038/srep19701
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Charge transport through one-dimensional Moiré crystals

Abstract: Moiré superlattices were generated in two-dimensional (2D) van der Waals heterostructures and have revealed intriguing electronic structures. The appearance of mini-Dirac cones within the conduction and valence bands of graphene is one of the most striking among the new quantum features. A Moiré superstructure emerges when at least two periodic sub-structures superimpose. 2D Moiré patterns have been particularly investigated in stacked hexagonal 2D atomic lattices like twisted graphene layers and graphene depo… Show more

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Cited by 23 publications
(27 citation statements)
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“…1 where τ e and τ sf are the free adjustable parameters, constant in energy, corresponding to the charge and spin lifetime; l e and l sf are the associated mean free paths; D and v are the charge carrier diffusion coefficient and velocity, respectively; DOS is the nanotube density of states per unit of length; and σ and ρ are the nanotube conductivity and resistivity, respectively. The energy-dependent density of states and charge carrier velocity of a pristine zigzag triple-wall CNT (TWCNT) of ~80 nm diameter, more precisely a (1045,0)@(1054,0)@(1063,0) TWCNT, were previously computed using tight-binding calculations in ( 60 ). All these quantities, as obtained with parameters τ e = 80 × 10 −12 s and τ sf = 10 4 × τ e = 800 × 10 −9 s, can be found in fig.…”
Section: Methodsmentioning
confidence: 99%
“…1 where τ e and τ sf are the free adjustable parameters, constant in energy, corresponding to the charge and spin lifetime; l e and l sf are the associated mean free paths; D and v are the charge carrier diffusion coefficient and velocity, respectively; DOS is the nanotube density of states per unit of length; and σ and ρ are the nanotube conductivity and resistivity, respectively. The energy-dependent density of states and charge carrier velocity of a pristine zigzag triple-wall CNT (TWCNT) of ~80 nm diameter, more precisely a (1045,0)@(1054,0)@(1063,0) TWCNT, were previously computed using tight-binding calculations in ( 60 ). All these quantities, as obtained with parameters τ e = 80 × 10 −12 s and τ sf = 10 4 × τ e = 800 × 10 −9 s, can be found in fig.…”
Section: Methodsmentioning
confidence: 99%
“…To understand the MPs, we use two methods: a simple superposition model (SSM) and an analytical model [75]. While approaches similar to our SSM have previously been applied in an ad-hoc way to several all-hexagonal systems [23,33,35,[77][78][79][80], here we demonstrate a consistent methodology that can in principle be applied to any system including those with mixed symmetry. MPs observed on α-Bi grown on HOPG have been successfully modeled previously using a commensurate model [44].…”
Section: Experimental and Modelingmentioning
confidence: 97%
“…While there has been a rapid progress on understanding the moiré physics in 2D heterostructures, experimental studies on moiré superlattice in one-dimensional (1D) systems are still limited, and no clear evidence on strong electronic structure modification has been made and explained in structure-identified 1D moiré superlattices [17][18][19][20]. Double-wall carbon nanotubes (DWCNTs), which correspond to a "rolled up" version of twisted bilayer graphene, naturally provide an ideal platform to experimentally probe the moiré physics in 1D.…”
mentioning
confidence: 99%